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2332-6 School on Synchrotron and FEL Based Methods and their Multi- Disciplinary Applications Peter Laggner 19 - 30 March 2012 University of Graz (Austria) Small-Angle X-Ray Scattering Fundamentals and Applications

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Page 1: School on Synchrotron and FEL Based Methods and their Multi- Disciplinary Applicationsindico.ictp.it/.../22/contribution/14/material/0/0.pdf · 2014-05-05 · 19.03.2012 1 Small-Angle

2332-6

School on Synchrotron and FEL Based Methods and their Multi-Disciplinary Applications

Peter Laggner

19 - 30 March 2012

University of Graz (Austria)

Small-Angle X-Ray Scattering � Fundamentals and Applications

Page 2: School on Synchrotron and FEL Based Methods and their Multi- Disciplinary Applicationsindico.ictp.it/.../22/contribution/14/material/0/0.pdf · 2014-05-05 · 19.03.2012 1 Small-Angle

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Small-Angle X-Ray Scattering –Fundamentals and Applications

Peter Laggner, Heinz Amenitsch, Michael Rappolt, Georg Pabst, Maria Schmuck, Benedetta Marmirolli, and Manfred Kriechbaum

ICTP School Trieste 210312March 19, 2012 1

CONTENTS

I. What is SAXS ?

II. General Areas of Application

III. Some Basic Physics

IV. Key Examples

V. Advanced Techniques / Synchrotron / Home-Laboratory

ICTP School Trieste 210312March 19, 2012 2

SAXNanoparticle Size and Shape,

10 – 1000 Å

WAXInner MolecularStructure

< 10Å

X-rays

< 5

> 5

ICTP School Trieste 210312March 19, 2012 3

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March 19, 2012 ICTP School Trieste 210312 4

The length scalesA Note on Scales

nm µm mm

Microporous Hydroxyapatite

This is where all the chemistry happens

Liposomal Carrier

The Product

This is our reality

x 106

SWAXS

log t (s)-6 -4 -2 0 2

Synchrotron beam-lines Lab-instruments

Typical Time-Scales

Small – Angle : Nano-Domain EnvelopeSize/Shape

The Reciprocity : Scattering Angle – Real Space Dimension

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SWAXS - simultaneous SAXS and WAXS

SAXS

1150 nm 10 3Angström

WAXScrystalline

amorphous

Nanometric density fluctuations

Nanoscale pores/ particles

Size - Shape

Atomic / molecularorder/disorder

Molecular packing

A blind-man‘s approach to SAXS:

Curve width: (reciprocal) size of inhomogeneities

Final slope: inner surface

Scattering angle

Inte

nsi

ty

Integral SAXS: domain volume

ICTP School Trieste 210312March 19, 2012 8

Specific inner surface, pore size

SAXS

WAXS Molecular crystal structure

SWAXS – simultaneous small-and wide angle scattering

ICTP School Trieste 210312March 19, 2012 9

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SAXS

WAXS

Molecular LatticeUnit cell dimensionssymmetry

Nano-EnvelopeSize / Shape

The angular resolution needs to be much better for SAXS than for XRD –

only ~ 6° ROI for two decades in real space

Why is SAXS special ?

ICTP School Trieste 210312

Nanomaterials

Structural Biology

Pharmacology

BiomaterialsNanocomposites

SWAXS Applications

March 19, 2012 11

Discovery Development Production Stability

•Proteomics

•HTP-screening

•Polymorph screening

•Hetero-Phase diagrams

•Controlled release

•QC

•PAT

•Aging

•Phase transitions

•Crystallization

Where can SAXS Provide Solutions for Chemistry ?

all these areasneed fast laboratory SAXS

Example Pharmaceutical Products

ICTP School Trieste 210312March 19, 2012 12

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SAXS – wherever nanostructure counts

Bulk powders

Liquid crystals

Biomaterials Polymers

Nanomaterials Proteins

SynchrotronLaboratory

Industry

Extreme conditions:

• fast kinetics – molecular movie

• thin film structure – GISAXS

• microfluidics

• micro- and nanobeams

• gas phase

• integration with other techniques

Tools for R&D, QC, PAT:

• constant availability

• speed and economy

• reliable, robust, automatisation

• on-line process control

• lab-GISAXS

• integration with other techniques

The main routes of development:

New techniques

New problems

The Routes of Innovation

ICTP School Trieste 210312March 19, 2012 14

The SAXS Experiment

source &monochromator

pinholes

sample

beam-stop

area-detector

c

Resolution1 - 100 nm

Other definitions:

ICTP School Trieste 210312March 19, 2012 15

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SAXS Theory

Fourier-integral

neutrons: b = nuclear scattering length(magnetic formfactor)

X-rays: b = atomic formfactor fZ

SAS: length scale >> atomic distances

Continuous scattering–length density

ICTP School Trieste 210312March 19, 2012 16

Two-phase Approximation

Two homogeneous phases ( and ) with sharp interfaces

Isotropic systems: spherical average

For isotropic systems (fluids, glasses, polycrystals)

no direction dependence of the scattered radiation

ICTP School Trieste 210312March 19, 2012 17

Two general laws

Integrated Intensity = volume fraction

Porods Law

S = total interface

per unit volume

Porod radiuse.g. <<1 and spherical particles

Rp = (/3) R R

ICTP School Trieste 210312March 19, 2012 18

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The four limiting cases

Dilute particles Crowded particles

Random porous/2-phase Liquid crystalline

ICTP School Trieste 210312March 19, 2012 19

Radius of gyration, particlesize, shape

Solution structure factor

Specific inner surface, pore size

Lattice dimensions, unit cell structure

ICTP School Trieste 210312March 19, 2012 20

Examples:

•Protein solutions

•Polymer solutions

•Nanoparticle solutions

Parameters

•Radius of Gyration

•Particle weight

•Particle Volume

Particle Shape

Dilute, Monodisperse System

ICTP School Trieste 210312March 19, 2012 21

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Rg = 15.5 Å

Solution SAX-Scattering of Lysozyme in 2% aqueous

Buffer:X-ray power: 2kW (CuKα), exposure-time: 1000 s

Background-subtracted raw-data of lysozyme (2%)

Guinier-Plot

q (Å-1)

Inte

nsi

ty (

cou

nts

)

q2

ICTP School Trieste 210312March 19, 2012 22

ICTP School Trieste 210312

Rapid Particle Sizing

lysozyme (2%)

q (Å-1)

Inte

nsi

ty (

cou

nts

)

q1/2 ~ 0.12 Å-1

Radius ~ π/ q1/2 ~ 26 Å

Poor-man‘s approach

March 19, 2012 23

The Pair Density Distribution Function p(R)

For globular particles:

Possible to determine :

maximum dimension of the particle

radius of gyration

zero-angle intensity

different particle geometries

ICTP School Trieste 210312March 19, 2012 24

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Crowded systemq

I

Experimental curve

S

q

P

q

Solution Structure Factor Particle Form Factor

x

ICTP School Trieste 210312March 19, 2012 25

Example:Particle Interaction

Scattering data are normalized to their concentration

ICTP School Trieste 210312March 19, 2012 26

SAXS is the most universal method for nanostructure analysis:

•Sensitive – low concentration (down to 0.1 %)

•Noninvasive – no preparation, staining or drying

•In-situ, real-time capabilities

•Extremely versatile (solids, liquids, gas phase)

The problem is how to retrieve the structural information from the scatteringpatterns

Principle of Solid-State SAXS

ICTP School Trieste 210312March 19, 2012 27

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The thermodynamic stability of a heterogeneous system (e.g. crystalline/amorphous) is not primarily determined by the percentage of the phases but by the interface per unit volume.

1 % amorphous can be harmless, or disatrous – depending on Si

The Solid-State Problem: Inner Surface

Lower inner surface

Higher stability

Higher inner surface

Lower stability

Equal %amorphous

or

porosity

ICTP School Trieste 210312March 19, 2012 28

SAXS

XRPD

µm

ICTP School Trieste 210312March 19, 2012 29

SAXS : A Measure of Stability

SAXS provides a measure for the specific inner surface(area per volume) between domains of different density

Density differences can arise from• Crystalline/amorphous domain structure• nanoporesBoth are thermodynamic instabilities: Gibbs‘ free

energy grows with inner surface area - the larger the inner surface, the lower the stability

ICTP School Trieste 210312March 19, 2012 30

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Recalling an old principle of small-angle scattering:

Porod, G. , Kolloid-Z. 124, 83 (1951)

l1

l2

l3

l4

ICTP School Trieste 210312March 19, 2012 31

l1

l2

l3

l4

The “Invariant“ Q:

The integral scattering, the ‚Invariant‘ , is equal to the total irradiated volume times the mean-square electron density

fluctuation – independent of domain shape. (Debye, Bueche)

Random porous/2-phase System

ICTP School Trieste 210312March 19, 2012 32

GENERAL RELATIONS (2)

In the case of a two-phase system ( e.g. crystalline/ amorphous polymer), the invariant is related to the

volume fractions , and the electron densities c and a

total irradiated volume

ICTP School Trieste 210312March 19, 2012 33

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GENERAL RELATIONS (3)

The decay constant k from a two-phase system is given by

K depends on the total inner surface and the mean-sqare electron density

fluctuations

ICTP School Trieste 210312March 19, 2012 34

ICTP School Trieste 210312

l1

l2

l3

l4

The inverse of k/Q is equalto the mean chordlength:

The mean pore diameters and wall diameters can be calculated from the relations:

and

March 19, 2012 35

How to obtain Si from experimental data:

• use the relation:

determine Porod limits from log I /log q –plot.

The slope should be –4 (at least close to that), according to I~q-4. If far from –4, system isfractal or has transition layer, and Si cannot be determined.

• determine K, from extrapolation to lg q = 0

• determine Q from integration (extrapolation to zero and infinity)

• Calculate Si in units of m2/g from :

p ... volume fraction of pores (e.g. He-pycnometry)

and s ... matrix density of the solid (e.g. crystal data).

ICTP School Trieste 210312March 19, 2012 36

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Comparison SAXS/BET

(BAM – Alumina Standards)

SAXS inner surface is higher than BET:

• inaccessible, closed pores

• nanostructured particle surface

Both are equally relevant for stability

Why?

BETm2/g

SAXSm2/g

PM-102 5,41 6,1

PM-104 79,8 97,4

PM-103 156,0 161,4

ICTP School Trieste 210312March 19, 2012 37

Inner surface by SAXS

... within minutes

....without drying

Mesoporous Materials - MCM

Nanomaterials

M.Lüchinger, G.Pirngruber, B.Lidlar, R.Prins and P. Laggner, J.Chem.Phys. (2004)

ICTP School Trieste 210312March 19, 2012 38

Monitoring Shape and Size of Pores in M41S Silicas

M.Lüchinger, G.Pirngruber, B.Lidlar, R.Prins and P. Laggner (2004)

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Synthesis procedure

dissolved silica (sodium silicate solution)

+ quaternary ammonium detergent micelles

organic, inorganic mesophase

mesoporous silica

100°C, 96 h 540°C in Air